Table of contents

Volume 7

Number 5, September 1998

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EDITORIAL

001

This special issue of Pure and Applied Optics is devoted to physical optics and coherence theory in honour of Professor Emil Wolf, one of the world's most distinguished scientists in these fields, whose 75th birthday fell on 30 July last year.

 

Professor Emil Wolf

Emil Wolf was born and grew up in Prague in Czechoslovakia. Being of Jewish origin, he fled the country after it was occupied by Nazi Germany in 1939. After brief periods in Italy and France (where he worked for the Czech government in exile), he arrived in Great Britain in the summer of 1940. He resumed his education the following year at the University of Bristol, where he earned a BSc degree in mathematics in 1945. It was as a postgraduate student that he began his studies in optics, designing the aspheric corrector [1]. After receiving a PhD degree from Bristol in 1948, he moved with his thesis supervisor, Dr E H Linfoot, to Cambridge University as a research assistant at the university observatory. It was during this period that he made several important contributions to the diffraction theory of aberrations [2] and to the study of the structure of optical fields in focal regions, a subject which he still continues to work on today. Also at that time his association with the exiled Hungarian scientist Professor Dennis Gabor began. Gabor, who was awarded the 1971 Nobel Prize in Physics for the invention of holography, was then at Imperial College. With the help of Gabor, Wolf obtained his next position, assistant to Nobel Laureate Max Born, who was then the Tait Professor of Mathematical Physics at the University of Edinburgh in Scotland. Born wanted to produce a revised English translation of his 1933 work Optik, and needed an assistant to help in this task. However, as the project progressed, the book evolved into an entirely more comprehensive and authoritative text. Since its publication in 1959 Principles of Optics by Max Born and Emil Wolf [3], or as it is more widely known `Born and Wolf', has become one of the most widely cited books in physical science, having been reprinted 15 times, and at the time of writing, a 7th edition is under preparation for publication by Cambridge University Press.

Following his years at Edinburgh (1951 - 54), from which university he received a DSc degree in 1955, Wolf was a research fellow at the University of Manchester (1954 - 59). Here Wolf published his seminal papers on coherence, a subject which he had begun investigating at Edinburgh. The theory of optical coherence, which had been largely originated by Fritz Zernike and others, was at that time a rather empirical series of formulae by which the visibility of interference fringes could be calculated. Wolf's 1955 paper [4] placed the theory on a firm theoretical basis, and established that the two-point correlation function obeys in free space the pair of wave equations

Also while at Manchester, Wolf worked with Brian Thompson, then a PhD student (who later became Director of the Institute of Optics and Provost of the University of Rochester), to produce a well-known experimental paper [5] which confirmed the calculations of fringe visibilities based on Wolf and Zernicke's earlier theoretical work.

In 1957 Wolf spent a sabbatical year at New York University, and in 1959 he was invited by Professor Robert Hopkins, director of the Institute of Optics, to join the faculty of the University of Rochester in New York State, where he has remained ever since, except for a year as a Guggenheim fellow at the University of California, Berkeley (1966 - 67), a year as a visiting Professor at the University of Toronto (1974 - 75) and a semester as a Distinguished Visiting Professor at the University of Central Florida (spring 1998). In recognition of his outstanding accomplishments, he was appointed to the Wilson Chair of Optical Physics at the University of Rochester in 1987. He has supervised (and continues to supervise) about 30 PhD students, including the editors of this special issue, many of whom have made contributions to this special issue, and also continues the regular academic activities of a full time professor of physics at the University of Rochester.

Wolf's work at Rochester in coherence theory, a good deal of it in collaboration with Professor Leonard Mandel, led to a classic review article on the subject in 1965 [6]. This article, which is one of the 100 most cited articles published by Reviews of Modern Physics since 1955, proved so popular that the authors decided to expand it into a full length book which finally appeared in 1995 [7]. His important investigations into the foundations of radiometry and its connection with coherence theory [8], and into the frequency representation of stationary random fields [9], led to the discovery of a new mechanism by means of which the spectrum of radiation can be changed on propagation even in free space. In particular, spectral lines can be shifted independently of the relative motion of the source and the observer [10]. This phenomenon, which has come to be known as `the Wolf effect', and is discussed in some of the articles of this special issue, may have very profound implications in cosmology. It also has applications to such fields as optical radiometric standards, communications and remote sensing (for a recent review of this subject, see [11]).

Other research areas that Professor Wolf has pursued include the reconstruction of objects from diffracted and scattered light: he published the seminal paper on diffraction tomography in 1969 [12]. He also continued his work on focused fields [13,14], and, with Y Li, gave the first explanation of the focal shift, by which the position of the focal spot can be displaced towards the focusing lens by diffractive effects [15]. He has also made important contributions to diffraction theory (for example the theory of the boundary diffraction wave [16]), the theory of non-radiating sources, phase retrieval in inverse problems and the Ewald - Oseen extinction theorem. Lack of space forbids us from citing all of his papers (over 280 at last count), so we have confined ourselves to mentioning a few representative examples of his work.

Professor Wolf has been awarded five honorary doctorates, from the University of Groningen, Netherlands (1989), from the University of Edinburgh, Scotland (1990), from Palacky University, Czechoslovakia (1992), from the University of Bristol, England (1997) and from Laval University, Canada (1997). In addition he is one of eight lifetime honorary members of the Optical Society of America, of which he served as president in 1978, and which he helped save from itself when it rather pointlessly attempted to change its name in 1989. He is also a fellow of the American Physical Society, the British Institute of Physics and the Franklin Institute and an honorary member of the Optical Society of India, the Optical Society of Australia and the Czech Academy of Sciences. He has also been the Editor since its founding in 1961 of the review series Progress in Optics, which now consists of 38 volumes, and he has also received many awards for his contributions, including the Ives Medal, the highest award of the Optical Society of America.

The subjects covered by the papers in this special issue, like Professor Wolf's research interests, range over a wide variety of fields. Many of the papers are written versions of talks presented at the Workshop on Physical Optics and Coherence Theory, also organized in honour of Professor Wolf, which was held at Long Beach, California, on 17 October 1997. We have arranged the papers into topical sections, as follows: coherence theory, the Wolf effect and spatial coherence spectroscopy, scattering and propagation in turbulent media, propagation in nonlinear media, propagation in dispersive media, periodicities in propagation, optical signal processing and the fractional Fourier transform, inverse problems and diffraction tomography, non-radiating sources, beam propagation and characterization and, finally, focused optical fields. In the spirit of fairness, the papers are arranged in these sections in the order in which they were received.

We are sure that we express the sentiments of all our contributors and readers when we wish Emil many more years of productive research. If there were any articles which were too late for inclusion in this special issue, we are most willing to consider them for the special issue we are planning for his 100th birthday in 2022, provided the article is likely to become of equally lasting value as those of Professor Wolf!

The editors would like to express their deep appreciation to Professor Mario Bertolotti, Michele Bouchareine and the editorial staff of the Journal of the European Optical Society, as well as to Tom Spicer, Elizabeth Martin and the staff of IOP Publishing for their untiring and highly professional help in preparing this special issue. This issue could not have been produced without the expert help of the various anonymous referees who reviewed the manuscripts.

  • [1] Wolf E and Preddy W S 1947 On the determination of aspheric profiles Proc. Phys. Soc. 59 704 - 11

  • [2] Wolf E 1951 The diffraction theory of aberrations Rep. Prog. Phys. 14 95 - 120

  • [3] Born M and Wolf E 1959 Principles of Optics (Oxford: Pergamon); reprinted 1998 6th edition (Cambridge: Cambridge University Press); Japanese translation 1974 - 75 (Tokyo: Tokai University Press). There have also been several unauthorized editions and translations: Russian 1970 (Moscow: Nauka); Chinese 1978 - 81 (Peking: Science); and various Taiwanese versions.

  • [4] Wolf E 1955 A macroscopic theory of interference and diffraction of light from finite sources II. Fields with a spectral range of arbitrary width Proc. R. Soc. A 230 246 - 65

  • [5]Thompson B J and Wolf E 1957 Two-beam interference with partially coherent light J. Opt. Soc. Am. 47 895 - 902

  • [6]Mandel L and Wolf E 1965 Coherence properties of optical fields Rev. Mod. Phys. 37 231 - 87

  • [7]Mandel L and Wolf E 1995 Optical Coherence and Quantum Optics (Cambridge: Cambridge University Press)

  • [8]Wolf E 1978 Coherence and radiometry J. Opt. Soc. Am. 68 6 - 17

  • [9] Wolf E 1981 New spectral representation of random sources and of the partially coherent fields that they generate Opt. Commun. 38 3 - 6

  • [10] Wolf E 1986 Invariance of the spectrum of light on propagation Phys. Rev. Lett. 56 1370 - 2 Wolf E 1987 Non-cosmological redshifts of spectral lines Nature 326 363 - 65

  • [11] Wolf E and James D F V 1996 Correlation-induced spectral changes Rep. Prog. Phys. 59 771 - 818

  • [12] Wolf E 1969 Three-dimensional structure determination of semi-transparent objects from holographic data Opt. Commun. 1 153 - 6

  • [13] Boivin A and Wolf E 1965 Electromagnetic field in the neighborhood of the focus of a coherent beam Phys. Rev. B 138 1561 - 5

  • [14] Wang W J, Friberg A T and Wolf E 1995 Structure of focused fields in systems of large Fresnel number J. Opt. Soc. Am. A 12 1947 - 53

  • [15] Li Y and Wolf E 1984 Three-dimensional intensity distribution near the focus in systems of different Fresnel numbers J. Opt. Soc. Am. A 1 801 - 8

  • [16] Miyamoto K and Wolf E 1962 Generalization of the Maggi - Rubinowicz theory of the boundary diffraction wave, Part I J. Opt. Soc. Am. 52 615 - 25 Miyamoto K and Wolf E 1962 Generalization of the Maggi - Rubinowicz theory of the boundary diffraction wave, Part II J. Opt. Soc. Am. 52 626 - 37

Guest Editors

Ari T Friberg Optics Section, Royal Institute of Technology, S-100 44 Stockholm, Sweden

Daniel F V James Theoretical Division T-4, Mail Stop B-268, Los Alamos National Laboratory, Los Alamos, NM 87545, USA

PAPERS

927

The concept of second-order anticoherence of two optical fields is defined via a cross-correlation function of the form . It is shown that the corresponding signal and idler fields produced in the process of parametric downconversion are mutually anticoherent, and it is pointed out that this anticoherence has already been observed experimentally, if somewhat indirectly.

933

, , and

We propose a high-precision digital automated quantitative determination of the modulus of the complex degree of coherence. The Thompson and Wolf experiment is repeated, using a CCD and a measurement method based on the fast Fourier transform. The experimental results agree very well with the predictions of the theory.

941

, , , and

We present an approach for describing the properties of a quasi-monochromatic, beam-like field that is both partially polarized and partially coherent from the spatial standpoint. It is based on the use of a single matrix, called the beam coherence-polarization matrix, whose elements have the form of mutual intensities. This approach, which can be viewed as an approximate form of Wolf's general tensorial theory of coherence, appears to be very simple, yet it is able to cover significant aspects of the beam behaviour that would not be accounted for by a scalar theory or by a local polarization matrix approach. A peculiar interference law applying to mutual intensities is derived. We show through simple examples how this approach leads to distinguish fields that would appear identical in a scalar treatment or in a local polarization matrix description. Hints for extensions are given.

959

We consider a simple model, based on currently accepted models for active galactic nuclei, for a quasi-stellar object (QSO or `quasar') and examine the influence that correlation-induced spectral changes (`the Wolf effect') may have upon the redshifts of the optical emission lines.

971

and

The theoretical foundation is described not only of how to determine the angular separation of two point spectral sources, but also on how to recover each spectral profile from the measured complex degree of spectral coherence. It is shown that the so-called space-frequency equivalence law is not always required. A simple simulation experiment is done by incorporating paired superluminescent diodes as the two point sources with different broadband spectra. The experimental results verify the validity of the theoretical prediction.

981

, , and

An interferometric technique based on the use of a diffraction grating is used to recover the intensity distribution across a spatially incoherent planar source. Information about the source profile is obtained through measurements of visibility and position of the fringe pattern at transverse planes beyond the grating. Such quantities are shown to be independent of the wavelength of the radiation, so that broadband sources can be analysed without any spectral filtering. Experimental results are given.

989

We show in this paper that the statistical properties of the speckle image formed at the focus of a large telescope can be fully described by a joint statistical analysis at N different spatial positions, where N is the number of resolution cells in the object's support. To obtain this result, the statistical properties are defined using multifold moment-generating functions (MGFs). Simplifying assumptions (discrete one-dimensional geometry, stationarity) are used to make the mathematical formalism simpler; they make the imaging process similar to a moving average process. General expressions are given for the twofold MGF and for MGFs of higher order. These relations are then used to show that an analysis of order N is exhaustive. It is shown that an MGF of order N + 1 can be written as the product of two MGFs of order N divided by an MGF of order N - 1. Alternatively, it is also shown that the cumulant of order N + 1 is equal to zero. A particular comment is made for the case of the double-star speckle pattern.

1001

and

Dynamics and light-scattering properties of Brownian particles in colloidal suspensions under the influence of the radiation pressure force of an illuminating laser beam are investigated by means of computer simulations using the Fokker-Planck equation and generalized Lorenz-Mie theory. Dynamic behaviour of the particles and a temporal correlation function of intensity fluctuations of the light scattered by these particles are calculated for various factors of particle size and power of the illuminating laser beam. Results of the simulations support the experimental observations of deformation in the temporal correlation functions of the scattered light and their dependences on the size of the particles and the power of the laser. From simulation results for the dynamics of particles, it is found that these changes in the correlation function arise from suppression of the random motion of the particles in the radial direction of the laser beam and induction of an average uniform motion in the beam propagation direction.

1013

and

Use of moments of non-integer order (called fractional moments) in statistical optics is proposed for discriminating between candidates for probability density functions (PDFs) of the scintillation intensity to overcome the experimental problems encountered by using integer moments. Low-order (< 2) fractional moments allow comparison of experimental data with theoretical PDFs of the intensity in different scintillation regimes. A comparison procedure, based on two low-order measured fractional moments, is described and tested by utilizing Monte Carlo samples from three distributions commonly used in atmospheric propagation (Ln, LnME and K). The bin width required to discriminate between different distributions and the effect of noise are investigated. Examples of application to experimental data are presented.

1033

, , and

An iterative method is developed to find exact solutions of wave propagation problems in Kerr media, taking into account backscattering effects. The method is based on the TE-mode Fourier-expansion eigenmode technique in the rigorous diffraction theory of gratings, but it permits an accurate treatment of non-periodic geometries as well. Self-focusing by a slab of Kerr medium is used to demonstrate the method and to compare it with the propagating-beam solution of the nonlinear Helmholtz equation, which ignores backscattering. The latter is shown to fail completely in many geometries, in particular, if the index modulation is high.

1043

and

The polarization properties of the phase-conjugate wave generated by means of degenerate four-wave mixing in isotropic Kerr-like media are analysed for monochromatic plane waves of arbitrary polarizations using the Laplace transformation to solve the coupled wave equations. The model presented enables us to find the reflection and transmission matrices defined for the electric and magnetic strength vectors and to discuss the efficiency and fidelity of the phase conjugation.

1053

, and

It is shown that the so-called paraxial approximation frequently used in nonlinear optics can break some conservation laws in the case of second harmonic generation.

1059

The angular spectrum of plane-waves representation of a pulsed electromagnetic beam field propagating in a dispersive, attenuative medium occupying the half-space expresses that wave field as a superposition of both homogeneous and inhomogeneous plane waves. A generalization of the Sherman expansion for source-free wave fields in lossless media to the lossy, dispersive medium case is used to derive a spatial series representation of a pulsed, source-free electromagnetic beam field from its angular spectrum representation. This spatial series representation displays the temporal evolution of the pulsed beam field explicitly through a single-contour integral that is of the same form as that obtained in the Fourier-Laplace description of a pulsed plane-wave field that is propagating in the positive z-direction in the lossy, dispersive medium. The temporal pulse evolution is found to depend upon the transverse spatial position in the beam field through the derivatives of the field boundary values.

1079

, and

We study the behaviour of a plane-wave delta-function pulse that is diffracted at an edge in a dispersive medium. In particular, we show that the edge-diffraction process by itself is dispersive and adds to the dispersion induced by the medium in such a way as to completely change the behaviour of the Brillouin precursor. The dispersion associated with edge diffraction manifests itself through the appearance of a new algebraic singularity near the origin. Since the Sommerfeld precursor field is due to asymptotic contributions from saddle points that always stay far from the origin, the character of this field is not changed by the new singularity induced by edge diffraction. The Brillouin precursor field, however, is due to asymptotic contributions from saddle points that are close to the origin, and therefore the new singularity changes its behaviour dramatically. Numerical illustrations of the evolution of the edge-diffracted pulse are given and the behaviour of the Brillouin precursor field is explained both mathematically and physically.

1103

, and

We present a general solution of the wave equation, obtained by the four-dimensional spectral method, for diffraction of a plane monochromatic light wave by a three-dimensional (3D) phase grating layer of finite thickness. As an example, we consider spherical particles in 3D phase gratings with orthogonal and hexagonal geometry. Conditions for the strong self-imaging of a 3D grating layer and for the weak self-imaging of a two-dimensional (2D) grating are formulated and investigated. Intensity distributions for diffracted light in planes of positive and negative self-imaging and in a plane of lowest contrast are computed and compared for 2D and 3D gratings. Some aspects of the Talbot and Lau effects for 2D and 3D phase gratings are discussed.

1121

, and

If a wave is laterally periodic, then it is also longitudinally periodic. Nevertheless, lateral periodicity is not needed for longitudinal periodicity. Lateral quasi-periodicity is a more general case and sufficient for longitudinal periodicity.

These results can be drawn from the Helmholtz equation, if the light is quasi-monochromatic and spatially coherent. For partially coherent light, similar results can be deduced from the Wolf equations.

The triple correlation of a complex amplitude obeys a pair of wave equations, which are constructed exactly like the Wolf equations. Hence, the same laws on periodicity are valid. We present a historical and systematic view of all of those periodicity laws.

1125

and

We present an optical algorithm for parallel multiplication of vectors and matrices using simple grating structures. The proposed scheme has the advantage that it does not require optical elements. Light while passing through the spatial light modulators, consisting of grating structures, gets multiplied and summed at the output plane. The scheme has the flexibility to perform matrix operations without changing the hardware.

1133

and

Effects of the aperture of a lens which is used to conduct an optical fractional Fourier transform on the fractional average intensity are analysed numerically using a computer. The fractional average intensity means the average intensity of the optical field produced from a partially coherent source in a fractional Fourier plane. In the present study, the fractional average intensities of a monochromatic Gaussian Schell model (GSM) source are evaluated using the root-mean square (RMS) difference between those with and without the effects of the lens aperture. It is clearly shown from our analysis that the aperture size of the lens should be twice as large as the GSM source size or greater in order to satisfy the condition of the RMS difference .

1143

We discuss how one can achieve subwavelength resolution using incident and scattered evanescent waves. We develop the underlying theoretical framework. We show how radiation from a dipole near a structure serves as its probe.

1151

The theory of diffraction tomography is generalized to random media. A relationship between the two-point spatial correlation function of the dielectric susceptibility and the cross-spectral density of the scattered field is derived, and the reconstruction of the two-point spatial correlation function from measurements of the cross-spectral density in two planes, on different sides and at finite distances from the medium, is investigated. It is shown that the two-point spatial correlation function cannot be determined uniquely, in general, from scattered field measurements, except for a class of random media known as quasi-homogeneous random media.

1161

, and

With applications in medical diagnosis in mind we apply the theory of diffraction tomography to diffuse photon density waves in a random medium. We consider the two-and-a-half-dimensional (2.5D) problem in which a two-dimensional (2D) object is illuminated by diffuse photon density waves from a point source. Both the forward problem and the inverse problem are discussed, and a reconstruction algorithm based on the weak-scattering approximation is presented together with computer simulations.

1181

, , , and

Starting from two-dimensional optical diffraction tomography (ODT) for an object embedded in a non-absorbing and non-scattering medium, we consider the case in which the object is embedded in a randomly scattering medium. We use the `effective wavenumber' K in the random medium and reasonable approximations to study both the forward problem and the inverse problem (i.e. the reconstruction of the object) and present relevant computer simulation results. For practical measurements of transmitted fields we discuss the possibility of using the coherent detection imaging (CDI) technique as a means of realizing ODT in a random medium.

1201

and

We separate the field generated by a spherically symmetric bounded scalar monochromatic source into a radiative and non-radiative part. The non-radiative part is obtained by projecting the total field on the space spanned by the non-radiating inhomogeneous modes, i.e. the modes which satisfy the inhomogeneous wave equation. Using residue techniques, introduced by Cauchy, we obtain an explicit analytical expression for the non-radiating component. We also identify the part of the source distribution which corresponds to this non-radiating part. The analysis is based on the scalar wave equation.

1213

and

The theory and results concerning the class of spherically symmetric non-radiating sources and fields established in an earlier paper by Gamliel et al are generalized to the non-spherically symmetric case. A procedure is described for constructing bases for the spaces of all non-radiating sources and associated fields confined to a spherical volume. An example is presented illustrating the developed theory.

1221

and

We consider the problem of the characterization of beams by moments of the field intensity in the aperture and its moments in the far field. The well known beam propagation factor, , is considered. We give convergence criteria for these factors and also discuss a new approach to optimization of the even moments of the far-field intensity.

1231

and

From the expansion of a partially coherent axially symmetric beam in terms of Laguerre-Gauss functions, we investigate the degree of accuracy reached by approaching the exact field by means of the lower-order terms of the above series. The accuracy is evaluated analytically as a function of both the number of terms of the expansion and the (measurable) second-order intensity moments of the beam, namely, the beam width and the so-called beam quality factor .

1237

, and

We study the problem of light focusing by a high-aperture lens through a planar interface between two media with different refractive indices. It is demonstrated how, by using annular illumination, the intensity distribution can be significantly confined. A new scanning mechanism is proposed to continuously probe the intensity peak through the second medium. This mechanism may be applied in, for example, lithography and three-dimensional imaging.

1249

, and

We study the propagation characteristics of focused, apertured radially symmetric beams and show that the axial point at which the mean-square radius of the diffracted beam is a minimum tends to be displaced towards the aperture plane depending on the Fresnel number associated with the aperture and the Fresnel number associated with the radius of the incident beam. The magnitude of this effect can be determined by a simple and general formula in terms of the amplitude distribution of the incident beam across the aperture and of the two Fresnel numbers. We investigate the focal shift effects for the case of a focused, apertured Gaussian beam. The irradiance and the encircled-power distributions in the plane at which the mean-square radius of the diffracted beam is minimum are calculated and compared with those corresponding to a uniform beam.